US4502008A - Method and apparatus for nuclear magnetic resonance spectroscopy - Google Patents

Method and apparatus for nuclear magnetic resonance spectroscopy Download PDF

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Publication number
US4502008A
US4502008A US06/465,324 US46532483A US4502008A US 4502008 A US4502008 A US 4502008A US 46532483 A US46532483 A US 46532483A US 4502008 A US4502008 A US 4502008A
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pulse
sub
pulse train
decoupling
radiofrequency
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Muneki Ohuchi
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Jeol Ltd
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Jeol Ltd
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    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R33/00—Arrangements or instruments for measuring magnetic variables
    • G01R33/20—Arrangements or instruments for measuring magnetic variables involving magnetic resonance
    • G01R33/44—Arrangements or instruments for measuring magnetic variables involving magnetic resonance using nuclear magnetic resonance [NMR]
    • G01R33/46—NMR spectroscopy
    • G01R33/4616—NMR spectroscopy using specific RF pulses or specific modulation schemes, e.g. stochastic excitation, adiabatic RF pulses, composite pulses, binomial pulses, Shinnar-le-Roux pulses, spectrally selective pulses not being used for spatial selection

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  • This invention relates to a method and apparatus for nuclear magnetic resonance spectroscopy, and more particularly to a method and apparatus for expanding the decoupling bandwidth.
  • spin decoupling technique is used for identifying or simplifying a spectrum split by spin-spin coupling and further for improving sensitivities.
  • spin decoupling is worked out by putting the unobserved nuclear species coupled with the observed nuclear species in a resonant state, and decoupling the spin-spin coupling, and basically, requires application of a radiofrequency magnetic field having the resonant frequency for the unobserved nuclear species.
  • application of a continuous wave radiofrequency field may result in a narrow decoupling bandwidth.
  • FIG. 1 shows the decoupling bandwidth according to each modulation method, where (a) refers to continuous irradiation without modulation; (b) refers to a case of noise modulation with a 1,000 Hz bandwidth; and (c) refers to a case of square wave phase modulation by 100 Hz square wave.
  • the nuclear species to be decoupled are protons and the resonant frequency (central frequency: 0 Hz off-set) is 100 MHz, and the peak power at (a) is normalized to 1.0.
  • the decoupling bandwidth in either case (b) or (c) can ultimately cover only about 1 KHz equivalent to the chemical shift width of protons at 100 MHz.
  • a pulse train which consists of 90° pulses (rf pulses having pulse width for rotating the magnetization by 90°) for the species to be decoupled and 240° pulses (rf pulses having pulse width for rotating the magnetization by 240°) without intervals, is applied repeatedly.
  • suffixes x, y, -x and -y indicate the phase of rf carrier in each pulse as follows: x: 0°; y: 90°; -x: 180°; and -y: 270°.
  • (d) represents the decoupling bandwidth obtained by the repeated irradiation of this pulse train.
  • the bandwidth becomes more than several times as broad as those obtained by any of the modulation methods shown in FIG. 1.
  • the peak strength also becomes higher than those obtained by the conventional decoupling methods, decoupling can be effectively complete over a wide range and the signal to noise ratio is improved.
  • This pulse decoupling method has been further advanced in the present invention. Namely, the present inventor has calculated the relations between the off-set frequency and J R /J 0 in the aforementioned pulse decoupling method under appropriate conditions.
  • the off-set frequency is the difference in frequency between the resonant frequency of the observed species and the resonant frequency of the species to be decoupled.
  • J 0 represents a distance between two peaks split by coupling and J R represents a distance between two peaks reduced by decoupling.
  • ⁇ I , ⁇ s are angular frequencies of I and S spin systems
  • I X , I Y , and I Z are X, Y, Z direction components of the magnetization of the I spin system
  • S X , S Y , S Z are X, Y, Z direction components of the magnetization of the S spin system
  • ⁇ I , ⁇ s are gyro-magnetic ratios of the spin systems I and S
  • J 0 is the coupling constant between I spin system and S spin system
  • II is the vector of the spins I
  • J R can be calculated according to this equation.
  • J R since rf field for decoupling is divided into pulses in the pulse decoupling method as shown in FIG. 2, J R must be first calculated at each pulse by dividing the time t into pulses; thereafter, J R can be averaged. Then J R /J 0 should be obtained.
  • FIG. 4 a solid line represents a result of the calculation according to the aforesaid process under appropriate conditions. From this figure, it is known that there are two peaks in the power distribution between zero off-set and 3 KHz off-set frequency, beyond which decoupling becomes progressively more incomplete.
  • the present inventor has discovered that it is possible to further expand the range of complete decoupling by elimination of these peaks. And based on repeated experiments, the present inventor has discovered that it is highly effective for expanding the complete decoupling range to combine the aforementioned pulse decoupling method with the square wave modulation method, namely, to reverse the phase (to shift 180° in phase) of rf carrier cyclically at a period longer than that of repetition of the pulse train.
  • the pulse train is not necessarily limited to what has been proposed by Freeman and many kinds of pulse trains can be contrived.
  • the results of calculations according to the present invention are shown in FIG. 4 by a broken line, wherein the abovementioned two peaks are eliminated and the line extends to roughly 4 KHz.
  • phase of the rf carrier is turned by 180° (the sign of suffix is reversed) in the middle of the pulse train.
  • the object of the present invention is to provide a method and apparatus for performing wide band decoupling.
  • FIG. 1 shows the bandwidth according to the prior art
  • FIG. 2 shows the arrangement of radiofrequency pulses in the pulse train proposed by Freeman
  • FIG. 3 shows the bandwidth according to the pulse decoupling method proposed by Freeman
  • FIG. 4 comprises plots showing J R /J 0 versus off-set frequency on the pulse decoupling method proposed by Freeman and on the method of the present invention
  • FIG. 5 is a block diagram of a nuclear magnetic resonance spectrometer incorporating features of the present invention.
  • FIG. 6 shows the measured bandwidths according to the present invention.
  • FIG. 7 shows the arrangement of radiofrequency pulses in an alternative pulse train.
  • an NMR probe 1 is arranged in a polarizing magnetic field.
  • Rf carrier for decoupling generated from rf oscillator 3 is transmitted to a specimen 2 at the probe 1 together with another rf for observation, and the free induction decay (FID) detected at the probe 1 is applied to a detection circuit (not shown) and processed therein.
  • the rf carrier for decoupling is provided with four different phases at a four-phase circuit 4, namely, 0°, 90°, 180° and 270° phases and subsequently sent to a selective circuit 5.
  • the selective circuit 5 selects the rf carrier with the desired phase for the desired duration of time and produces pulse trains.
  • the pulse trains are phase modulated at a modulator 8 to which a square wave signal is supplied from a square wave oscillator 7.
  • the output of modulator 8 is supplied to the probe 1 through a power amplifier 9 and transmitted to the specimen.
  • the pulse programmer 6 already has the information regarding the phase and pulse width for all rf pulses contained in the pulse train, in the order of irradiation.
  • each rf pulse is converted to the information of the phase of rf carrier and pulse width as follows:
  • an operator can prepare any kind of pulses having arbitrary pulse width and can also specify the phase of the rf carrier at 0°, 90°, 180°, or 270°; therefore, he can prepare any kind of pulse train by joining any number and any kind of pulses.
  • solid line (e) shows the bandwidth under the condition that the pulse train shown in FIG. 2 applied repeatedly and phase-modulated asynchronously with a square wave of 100 Hz, chosen here to be a longer period than that of the pulse train. It is obvious from this figure, that by adding the square wave phase-modulation, the bandwidth of rf field for decoupling is expanded from 8 KHz in FIG. 3 to 11 KHz in FIG. 6 by comparison at the level of 0.5 on the axis of ordinates.
  • solid line (f) shows the bandwidth obtained by the pulse train shown in FIG. 7. It is obvious from this figure that the bandwidth spreads over 16 KHz.
  • any pulse train in which at least either of two unit pulse trains R +1 and R +1' and either of two unit pulse trains R -1 and R -1' , are contained, can be used.
  • R +1 represents a unit pulse train in which A° x pulse, B° y pulse and A° x pulse are combined in this order
  • R -1 represents a unit pulse train in which A° -x pulse, B° -y pulse and A° -x pulse are combined in this order
  • R +1' represents a unit pulse train in which A° x pulse and B° y pulse are combined in this order
  • R -1' represents a unit pulse train in which A° -x pulse and B° -y pulse are combined in this order.
  • a and B of the A° pulse and B° pulse can be chosen ranging from about 90 to 45 and B can be chosen ranging from 240 to 90.
  • the other some pulse, C° pulse having a different pulse width from the A° pulse and B° pulse can be optionally combined in the sequence.
  • the range of decoupling can be expanded according to the present invention. Therefore, the following excellent effects can be obtained: (1) nuclear species with large chemical shifts such as 19 F are easily decoupled, (2) wide range decoupling can be worked out in NMR spectrometers with resonant frequency of 400 MHz or higher, (3) since wide range decoupling is possible with low decoupling power, the construction of power amplifiers and the related circuits can be simplified, (4) a field of applications is expanded, because samples which could not be measured on account of intolerable heating by decoupling power can be measured, (5) not only the signal to noise ratio but also quantification are improved because broadband and uniform decoupling can be worked out according to the present invention.
  • the modulator 8 may be arranged between the oscillator 3 and the four-phase circuit 4 to modulate rf carrier for decoupling.

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  • Physics & Mathematics (AREA)
  • Spectroscopy & Molecular Physics (AREA)
  • High Energy & Nuclear Physics (AREA)
  • Condensed Matter Physics & Semiconductors (AREA)
  • General Physics & Mathematics (AREA)
  • Magnetic Resonance Imaging Apparatus (AREA)
US06/465,324 1982-02-19 1983-02-09 Method and apparatus for nuclear magnetic resonance spectroscopy Expired - Lifetime US4502008A (en)

Applications Claiming Priority (2)

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JP57-25492 1982-02-19
JP57025492A JPS58142251A (ja) 1982-02-19 1982-02-19 核磁気共鳴測定方法

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DE (1) DE3304798A1 (de)
GB (1) GB2117119B (de)

Cited By (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4613949A (en) * 1984-02-17 1986-09-23 General Electric Company Composite pulses for time reversal in NMR imaging
US4641096A (en) * 1983-11-30 1987-02-03 Jeol Ltd. Nuclear magnetic resonance spectrometry
US4651097A (en) * 1983-10-12 1987-03-17 Yokogawa Hokushin Electric Corporation Examination method and apparatus utilizing nuclear magnetic resonance
US4683432A (en) * 1985-09-25 1987-07-28 Picker International, Inc. Nuclear magnetic resonance methods and apparatus
US4736328A (en) * 1985-09-23 1988-04-05 General Electric Company Apparatus for shifting the phase of transmitter and receiver analog baseband signals in an NMR system
US4891593A (en) * 1987-08-05 1990-01-02 National Research Development Corporation Methods of obtaining images representing the distribution of paramagnetic molecules in solution
US5041790A (en) * 1990-01-16 1991-08-20 Toshiba America Mri, Inc. Dual-tuned RF coil for MRI spectroscopy
US5196795A (en) * 1988-11-25 1993-03-23 Spectrospin Ag Method for selective excitation of nmr signals
US10502802B1 (en) 2010-04-14 2019-12-10 Hypres, Inc. System and method for noise reduction in magnetic resonance imaging

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4068161A (en) * 1976-05-13 1978-01-10 Varian Associates, Inc. Gyromagnetic resonance spectroscopy employing spin echo spin-spin decoupling and two-dimensional spreading

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE2126743C3 (de) * 1971-05-28 1974-05-16 Spectrospin Ag, Faellanden (Schweiz) Verfahren zur Aufnahme von Spin- ' resonanzspektren

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4068161A (en) * 1976-05-13 1978-01-10 Varian Associates, Inc. Gyromagnetic resonance spectroscopy employing spin echo spin-spin decoupling and two-dimensional spreading

Non-Patent Citations (2)

* Cited by examiner, † Cited by third party
Title
R. Freeman et al., "Composite Pulse Decoupling" Journal of Magnetic Resonance, 43, pp. 502-507 (1981).
R. Freeman et al., Composite Pulse Decoupling Journal of Magnetic Resonance, 43, pp. 502 507 (1981). *

Cited By (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4651097A (en) * 1983-10-12 1987-03-17 Yokogawa Hokushin Electric Corporation Examination method and apparatus utilizing nuclear magnetic resonance
US4641096A (en) * 1983-11-30 1987-02-03 Jeol Ltd. Nuclear magnetic resonance spectrometry
US4613949A (en) * 1984-02-17 1986-09-23 General Electric Company Composite pulses for time reversal in NMR imaging
US4736328A (en) * 1985-09-23 1988-04-05 General Electric Company Apparatus for shifting the phase of transmitter and receiver analog baseband signals in an NMR system
US4683432A (en) * 1985-09-25 1987-07-28 Picker International, Inc. Nuclear magnetic resonance methods and apparatus
US4891593A (en) * 1987-08-05 1990-01-02 National Research Development Corporation Methods of obtaining images representing the distribution of paramagnetic molecules in solution
US5196795A (en) * 1988-11-25 1993-03-23 Spectrospin Ag Method for selective excitation of nmr signals
US5041790A (en) * 1990-01-16 1991-08-20 Toshiba America Mri, Inc. Dual-tuned RF coil for MRI spectroscopy
US10502802B1 (en) 2010-04-14 2019-12-10 Hypres, Inc. System and method for noise reduction in magnetic resonance imaging

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Publication number Publication date
GB2117119A (en) 1983-10-05
JPS622261B2 (de) 1987-01-19
JPS58142251A (ja) 1983-08-24
GB8302845D0 (en) 1983-03-09
GB2117119B (en) 1986-01-02
DE3304798A1 (de) 1983-09-22

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